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中国物理学会期刊

基于神经网络波函数的粲偶素势模型研究

Study of charmonium potential models based on neural network wave functions

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  • 本研究基于神经网络波函数发展了一套完整的粲偶素势模型参数拟合框架,旨在解决传统唯象势模型参数难以快速响应实验进展的问题。该方法将神经网络波函数作为径向薛定谔方程的变分解,通过显式构造节点因子与残差网络结构,精确求解粲偶素体系的基态与激发态;在此基础上,采用最大似然估计以及拉普拉斯近似对势模型参数进行推断,以获得最优参数及其不确定度。应用该框架对粲偶素势模型的五个势参数进行联合优化,优化后参数为:正反粲夸克质量mc=mc=1.4801 ± 0.0055 GeV,强相互作用耦合常数αs=0.5459 ± 0.0120,弦张力σlin=0.1442 ±0.0028 GeV2,涂抹半径σsmear=1.1047 ± 0.0568 GeV。相比于原始参数,优化后模型对16个已知粲偶素态的均方根偏差(RMSD)从26.26 MeV降至24.62 MeV。基于优化参数预测了包括S、P、D、F波在内的粲偶素质量谱,结果符合势模型理论预期,预测的高角动量态为未来实验搜寻提供了理论参考。

     

    This study presents a comprehensive framework for fitting the phenomenological potential model parameters of charmonium by integrating neural network wavefunctions. This approach overcomes the limitations of traditional fitting methods, which adapt slowly to new experimental data. In this method, the radial Schrödinger equation is solved variationally using a neural network wavefunction ansatz. The wavefunction incorporates an explicitly constructed node factor that accurately represents the nodal structure of excited states. It also employs a residual network architecture to enhance expressiveness and training stability. The number of nodes is specified according to the target radial excitation, while the node positions are treated as trainable parameters, enabling the neural network to optimize the excited-state wavefunctions without preassigning their nodal locations. The energy variance is used as the training objective, and automatic differentiation is employed to calculate the derivatives required in the variational optimization and subsequent parameter inference. After determining the eigenwavefunctions and eigenenergies, the potential parameters are inferred via maximum likelihood estimation with the Laplace approximation, yielding optimal parameter values and their uncertainties. In the likelihood construction, a fixed theoretical uncertainty is introduced together with the experimental errors so that the fitting procedure reflects both experimental precision and the intrinsic approximation of the potential model. The method is applied to a phenomenological charmonium potential that includes a Coulomb term, a linear confinement term, a smeared spin-spin interaction, and spin-orbit and tensor forces treated perturbatively. The fitted parameters are the charm quark mass mc = mc = 1.4801 ±0.0055 GeV, the strong coupling constant αs = 0.5459 ±0.0120, the string tension σlin = 0.1442 ±0.0028 GeV2, and the smearing radius σsmear = 1.1047±0.0568 GeV. Compared with the original parameters, the optimized model improves the agreement with the 16 known charmonium states from the Particle Data Group. The root-mean-square deviation is reduced from 26.26 MeV to 24.62 MeV. Based on the optimized parameters, the mass spectrum of charmonium is predicted up to high excitation levels, including S, P, D, and F waves. The predicted energy level spacings and fine structures are consistent with the expected behavior of the confining potential, indicating that the optimized parameters retain the main physical features of the conventional potential model. Notably, the framework provides predictions for unobserved high-angular-momentum states such as the n3FJ and n1F3 series, which may serve as references for future experimental searches at facilities such as BESIII, Belle II and LHCb. The main innovation of this work is to combine neural network wavefunctions with statistical parameter inference, so that the solution of the Schrödinger equation, the fitting of potential parameters, and the quantification of parameter uncertainties are incorporated into an automated and extensible workflow. The proposed framework can be readily extended to other heavy quark systems such as bottomonium and Bc mesons, as well as to more complex spectroscopic problems involving coupled-channel effects.

     

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